“…Stone has presented a rigorous theory for describing polarization that gives excellent results on small molecules , but, the method is not readily applicable to large biomolecular systems. For such systems, the usual simplification is to assign point charges, q , and isotropic scalar polarizabilities, α, to the atoms; here, as elsewhere, , we used the isotropic atomic polarizabilities of Miller and Savchik . The field, E , due to the point charges, q (and the induced dipoles, μ), then gives rise to induced dipoles, μ, via
The induced dipoles, μ, modify the field, E , and so eq 1 is usually solved by iteration, but considerable improvement in accuracy can still be obtained without iteration − and hence with consequent savings in CPU time.…”