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Reviews in Computational Chemistry Volume 18

Reviews in Computational Chemistry Volume 18

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CHAPTER 3<br />

Potentials and Algorithms for<br />

Incorporat<strong>in</strong>g Polarizability <strong>in</strong><br />

Computer Simulations<br />

Steven W. Rick* and Steven J. Stuart y<br />

*Department of <strong>Chemistry</strong>, University of New Orleans,<br />

New Orleans, Louisiana 70148 and <strong>Chemistry</strong> Department,<br />

Southern University of New Orleans, New Orleans, Louisiana<br />

70126, and y Department of <strong>Chemistry</strong>, Clemson University,<br />

Clemson, South Carol<strong>in</strong>a 29634<br />

INTRODUCTION<br />

<strong>Reviews</strong> <strong>in</strong> <strong>Computational</strong> <strong>Chemistry</strong>, <strong>Volume</strong> <strong>18</strong><br />

E dited by K enny B. L ipkowitz and D onald B. Boyd<br />

Copyr ight © 2002 John Wiley & Sons, I nc.<br />

ISBN: 0-471-21576-7<br />

Polarization refers to the redistribution of a particle’s electron density<br />

due to an electric field. In terms of molecular <strong>in</strong>teractions, polarization leads<br />

to nonadditivity, s<strong>in</strong>ce a molecule polarized by another molecule will <strong>in</strong>teract<br />

differently with a third molecule than it would if it were not polarized. The<br />

change <strong>in</strong> the electron density can be characterized by changes <strong>in</strong> the monopole<br />

charges, dipole moments, or higher order moments. Methods for treat<strong>in</strong>g<br />

polarizability <strong>in</strong> molecular dynamics or Monte Carlo simulations achieve this<br />

goal through <strong>in</strong>ducible dipole moments (the polarizable po<strong>in</strong>t dipole and shell<br />

models) or through fluctuat<strong>in</strong>g charges (the electronegativity equalization and<br />

semiempirical models). This chapter describes these models, with a focus on<br />

those methods that have been developed for molecular dynamics and Monte<br />

89

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