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Introduction to Force Fields

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4<br />

The Electrostatic Energy<br />

The Coulomb interaction potential between two charged particles is<br />

U el =<br />

q A q B<br />

4πε 0 r AB<br />

, (7)<br />

€<br />

where q A and q B are the charges on particles A and B and r AB is the distance between a<strong>to</strong>ms A and B. The<br />

attractive interaction between opposite charges in shown in Figure 5(a) and the repulsive interaction between like<br />

€<br />

charges is shown in Figure 5(b).<br />

€<br />

€<br />

Electrostatic Energy<br />

Electrostatic Energy<br />

0 2 4 6 8 10<br />

r AB (Å)<br />

0 2 4 6 8 10<br />

r AB (Å)<br />

(a) (b)<br />

Figure 5. Typical behavior of the electrostatic energy for (a) opposite charges and (b) like charges.<br />

Determination of <strong>Force</strong> Field Parameters<br />

The parameters that make up the force field generally are derived from experimental data. This can be done in many<br />

different ways; thus, there are many different force fields available in the literature. Some have been constructed <strong>to</strong><br />

deal with small organic molecules, others have been generated <strong>to</strong> focus especially on biomolecules, and others are of<br />

general utility.<br />

Sample <strong>Force</strong> Field Parameters<br />

Molecular mechanics (MM) calculations rely on force fields constructed from empirical data. The force field<br />

parameters are obtained from experimental or quantum mechanical results. Shown in Tables 1 and 2 are some<br />

example bond stretching and angle bending force field parameters. These parameters are from the MM3 force field.<br />

Table 1. Example bond stretching parameters, MM3 force field<br />

Bond type<br />

r AB,eq<br />

k s,AB<br />

(Å)<br />

(kJ mol –1 Å –2 )<br />

Csp 3 –Csp 3 €<br />

1.523<br />

€<br />

1330<br />

Csp 3 –Csp 2 1.497 1330<br />

Csp 2 =Csp 2 1.337 2890<br />

Csp 2 =O 1.208 3250<br />

Csp 3 –Nsp 3 1.438 1540<br />

Note that the stretching force constants for double bonds are in general larger than the stretching force constants for<br />

single bonds.

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