Alternative name: (empirical) force field calculations
Definition: "a calculational method to give accurate a
priori structures and energies for molecules" [Allinger]
Based on classical-mechanical model of molecular structures
(it is assumed that a set of equations exist which are of the form of the
classical equations of motions)
Energy of a molecule is represented as the sum of contributions due to
bond stretching, bond bending, van der Waals attractions and repulsions between
nonbonded atoms, electrostatic interactions due to polar bonds, and energy
changes accompanying internal rotation about single bonds
Molecular mechanics calculations produce:
(1) equilibrium structures (and transition states)
(2) energies: strain energies and heats of formation
(3) vibrational frequencies
| Andrews | 1930 | basic ideas from
vibrational spectroscopy |
| Hill | 1946 | include van der
Waals interactions in |
| Westheimer and Mayer | 1946 | application: racemization |
| Dostrovsky, Hughes, Ingold | 1946 | application: SN2
reaction |
| Hendrickson | 1960 | utilize computer |
| Wiberg | 1965 | first general
computer program |
| Allinger | 1973 | MM1 (first MM package) |
| Allinger | 1977 | MM2 & MMP2 |
| Allinger | 1989 | MM3 |
| commercial companies | 1990 |
molecular modelling software with |
| academics and companies | 1990s | universal force fields |
Mechanical model: a molecule is considered to be a series of masses (atoms)
attached by springs (bonds)
A molecule can be described by a collection of atomic nuclei
distribution on a potential energy surface
Born-Oppenheimer approximation:
one can consider separately the motions of electrons and the motion of nuclei,
because of their large difference in mass
(1) quantum mechanics: consider the electron explicitly and the
potential energy function is a sum of the nuclear energy and the electronic
energy obtained by an approximation solution of the electronic Schrödinger
equation
(2) molecular mechanics: electrons are not considered explicitly
and the potential energy of a molecule is a function of geometrical variables
and the parameters of the model are chosen to fit experimental data
Potential energy surface of a molecule with n atoms (3n coordinates) can be
approximated by a Taylor series expansion about the point of minimum
energy (V0) in terms of displacement coordinates and derivatives of the potential
energy (valid for small displacement)
di,
dj
and dk
= displacement coordinates
fi,
fij
and fijk
= first, second
and third derivatives with respect to displacement coordinates
From the analysis of vibrational spectrum, it is possible to
derive force constants
Harmonic force field: motion in each of the coordinates is independent of motion
in the others, i.e. the force constant matrix is diagonal

Total energy of a molecule is the sum of bond stretch, angle
bend, torsional and nonbonded contributions, etc.
Definition: a force field is an empirical fit to a Born-Oppenheimer
potential energy surface
One must select the coordinate to be used, the functional
form(s) of the energy in terms of the coordinates, and the function parameters
Force fields are determined by parameterizing potential
energy functions so that it can reproduce a range of properties for stable
molecules (both experiments and high-level ab initio results)