Molecular Mechanics Notes
(Leach - Ch 3; Grant & Richards, Ch. 3)
- empirical potentials fitted to experimental and calculational data
- composed of stretches, bend, torsion and non-bonded components (e.g.
stretch component has a term for each bond in the molecule)
- potential energy curves for individual terms are approximately transferable
(e.g. CH stretch in ethane almost the same as in octane)
- terms consist of functional forms and parameters
- parameters chosen to fit structures (in some cases also vibrational
spectra, steric energies
- each atomic number divided into atom types, based on bonding and environment
(e.g. carbon: sp3, sp2, sp, aromatic, carbonyl, etc.)
- parameters assigned based on the atom types involved (e.g. different
C-C bond length and force constant for sp3-sp3 vs
sp2-sp2)
- force field comprised of functional forms, parameters and atom types
- examples: MM2, MM3, Amber, Sybyl, Dreiding, UFF, MMFF, etc.
- some force field use united atoms (i.e. H's condensed into the heavy
atoms) to reduce the total number of atoms (but with a reduction in accuracy)
- do not mix and match - each developed to be internally self consistent
- MM force fields differ from force fields used for vibrational analysis,
and analytical potential energy surfaces used for dynamics - these are
custom fit for individual systems
- MM force fields are designed to be transferable, and can be used for
broad classes of molecular systems (but stay within the scope of the original
parameterization)
Bond Stretch term
- many use just quadratic term, but too large for very elongated bonds
- Morse (usually not used because of expense), cubic (wrong asymptotic
form), quartic
- reference bond length not the same as the equilibrium bond length,
because of non-bonded contributions
Angle Bend term
- usually quadratic is sufficient
- special atom type may be used for very strained atoms (e.g. cyclopropane)
Torsion term
- most use a single cosine with appropriate barrier multiplicity
- some use a sum of cosines for 1-fold (dipole), 2-fold (conjugation)
and 3-fold (steric) contributions
- improper torsions used for out-of-plane bends (and chirality constraints
in united atom force fields)
Non-bonded term
- van der Waals interactions
- repulsive part - overlap of electron distributions - Pauli exclusion
- attractive part - London or dispersion forces
- instantaneous dipole - induce dipole interaction r -6
- Lennard-Jones: 4 epsilon ( (sigma / r)12 - (sigma / r)6)
(easy to compute, but r -12 rises too rapidly)
- Buckingham: A exp(-Br) - C r-6 (QM suggests exp repulsion
better, but is harder to compute)
- tabulate s and e for each atom - mixed terms: sigmaAB =
(sigmaAA + sigmaBB)/2; epsilonAB
= (epsilonAA epsilonBB)1/2
Electrostatics
- charges can be obtained from MO calculations (expensive, some difficulties)
- atom centered charges obtained by fit to ESP - may vary with conformation
- can also include atom centered multipoles for better fit to ESP
- possibly use off-center charges for better representation of ESP around
lone pairs
- cheaper (but less accurate) method for calculating charges - electronegativity
equalization
- polarization effects - compute iteratively (expensive and not that
much of an improvement)
- include polarization effects in an average way with distance dependent
dielectric constant
Hydrogen bonding
- some force fields add extra term: A/r12 - C/r10
- others just use a balance between electrostatic and non-bonded terms
Parameterization
- difficult, computationally intensive, inexact
- fit to structures (and properties) for a set of molecules
- recent generation of force fields fit to ab initio data at minima and
distorted geometries
- trial and error fit, or least squares fit
- different parameter sets and functional forms can give similar structures
and energies
- don't mix and match
Energencies
- steric energy - energy relative to an artificial structure with no
interactions - can be used to compare different conformers of same molecule
- strain energy - energy relative to a strainless molecule - e.g. all
trans hydrocarbons
- heat of formation - average bond energies added to energy t get approximate
atomization energy
- very dangerous to decompose steric energy into components
- different force fields can give similar energies and structures but
quite different components
Applications
- geometry and relative energies of conformers of the same molecule
- effect of substituents on geometry and strain energy
- well parameterized for organics, less so for inorganics
- specialty force fields for proteins, DNA, for liquid simulation
- molecular mechanics cannot be used for reactions that break bonds
- simple organic problems: ring strain in cycloalkanes, conformational
analysis, Bredt's rule
- high end biochemistry problems: docking of substrates into active sites,
refining x-ray structures, determining structures from NMR data, free energy
simulations