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Charge-Dipole Interaction<br />

Term<br />

Allinger’s potential function includes one of two<br />

possible electrostatic terms: one based on bond<br />

dipoles, or one based on partial atomic charges. The<br />

addition of a charge-dipole interaction term allows<br />

for a combined approach, where partial charges are<br />

represented as bond dipoles, and charged groups,<br />

such as ammonium or phosphate, are treated as<br />

point charges.<br />

Quartic Stretching Term<br />

With the addition of a quartic bond stretching term,<br />

troublesome negative bond stretching energies<br />

which appear when long bonds are treated by<br />

Allinger’s force field are eliminated.<br />

The quartic bond stretching term is required<br />

primarily for molecular dynamics; it has little or no<br />

effect on low energy conformations.<br />

To precisely reproduce energies obtained with<br />

Allinger’s force field:<br />

• Set the quartic stretching constant in the MM2<br />

Constants table window to zero.<br />

The quartic term is eliminated.<br />

Electrostatic and van der<br />

Waals Cutoff Terms<br />

The cutoffs for electrostatic and van der Waals<br />

terms greatly improve the computation speed for<br />

large molecules by eliminating long range<br />

interactions from the computation.<br />

To precisely reproduce energies obtained with<br />

Allinger’s force field:<br />

• Set the cutoff distances to large values (greater<br />

than the diameter of the model).<br />

Every interaction is then computed.<br />

The cutoff is implemented gradually, beginning at<br />

50% of the specified cutoff distance for charge and<br />

charge-dipole interactions, 75% for dipole-dipole<br />

interactions, and 90% for van der Waals<br />

interactions. Chem3D uses a fifth-order polynomial<br />

switching function so that the resulting force field<br />

is second-order continuous.<br />

Because the charge-charge interaction energy<br />

between two point charges separated by a distance<br />

r is proportional to 1/r, the charge-charge cutoff<br />

must be rather large, typically 30 or 40Å. The<br />

charge-dipole, dipole-dipole, and van der Waals<br />

energies, which fall off as 1/r 2 , 1/r 3 , and 1/r 6 ,<br />

respectively, can be cut off at much shorter<br />

distances, for example, 25Å, 18Å, and 10Å,<br />

respectively. Fortunately, since the van der Waals<br />

interactions are by far the most numerous, this<br />

cutoff speeds the computation significantly, even<br />

for relatively small molecules.<br />

Pi Orbital SCF <strong>Com</strong>putation<br />

Chem3D determines whether the model contains<br />

any pi systems, and performs a Pariser-Parr-Pople<br />

pi orbital SCF computation for each system. A pi<br />

system is defined as a sequence of three or more<br />

atoms of types which appear in the Pi Atoms table<br />

window (PIATOMS.xml).<br />

The method used is that of D.H. Lo and M.A.<br />

Whitehead, Can. J. Chem., 46, 2027 (1968), with<br />

heterocycle parameters according to G.D. Zeiss<br />

and M.A. Whitehead, J. Chem. Soc. (A), 1727 (1971).<br />

The SCF computation yields bond orders which are<br />

used to scale the bond stretching force constants,<br />

standard bond lengths, and twofold torsional<br />

barriers.<br />

A step-wise overview of the process used to do pi<br />

system calculations is as follows:<br />

5. A matrix called the Fock matrix is initialized to<br />

represent the favorability of sharing electrons<br />

between pairs of atoms in a pi system.<br />

Appendices<br />

<strong>ChemOffice</strong> 2005/Appendix MM2 • 673<br />

Chem3D Changes to Allinger’s Force Field

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