Solvation Free Energy of Biomacromolecules: Parameters for a Modified Generalized Born
Model Consistent with the AMBER Force Field
B. Jayaram,
†
D. Sprous, and D. L. Beveridge*
Department of Chemistry, Wesleyan UniVersity, Middletown, Connecticut 06459
ReceiVed: April 27, 1998
The generalized Born (GB) model provides rapid estimates of the electrostatic free energies of solvation for
diverse molecules and molecular ions. This method is expected to be of considerable utility for studies of
solvation in macromolecular and biological systems. Calculations on biological molecules are typically based
on empirical energy functions, each of which have their own prescriptions for determining net atomic charges.
For maximum compatibility, GB parameters tailored to specific force fields are required. The development
of parameters compatible with the AMBER force field is described. The method is used to estimate free
energies of A and B form structures of DNA obtained from molecular dynamics simulations. The results
provide an account of the conformational preferences of right-handed DNA in solution.
I. Introduction
Generalized Born (GB) theory
1-4
is the basis of a computa-
tional method for estimating the electrostatic free energies of
solvation of diverse molecules and molecular ions. In the GB
model, a molecule in solution is represented as a set of point
charges set in spherical cavities embedded in a polarizable
dielectric continuum. GB calculations can be considered as a
means of approximating finite difference Poisson-Boltzmann
5
free energies and related quantities. Previous studies have
demonstrated that the GB method together with a simple
treatment of nonelectrostatic effects can estimate solvation free
energies that are generally within 5% of observed values,
1,4
and
a recent modification, the MGB method,
6
has extended the
purview of the GB theory to pK shifts of dicarboxylic acids as
well as hydration energies.
The essential simplicity of the GB method results in rapid
computation times in numerical calculations, and thus its
extension to macromolecular and biological solvation problems
is readily feasible. However, macromolecular energy calcula-
tions are typically based on empirical energy functions such as
AMBER,
7
CHARMM,
8
or GROMOS,
9
each of which have their
own prescription for specifying the net atomic charges on the
individual atoms of the system. For a GB model to be
successful on these systems, it is necessary that the effective
GB radii for each atom type be parametrized in a manner fully
consistent with the net atomic charges intrinsic to the assumed
energy function. We describe herein the nature of the reparam-
etrization process necessary to achieve this consonance and
report the parameters required to obtain the effective Born radii
compatible with the recently proposed force field of Cornell et
al.,
10
incorporated into the AMBER suite of programs.
7
The
reparametrized GB model is found to reproduce solvation free
energies of 32 molecules, chosen as prototypes of protein and
nucleic acid constituents, with a mean unsigned error of <1
kcal. Preliminary application of the method to treat the solvent
dependent conformational preferences of a right-handed B-DNA
double helix is described.
II. Background
The generalized Born model treats a molecule as a discrete
set of overlapping charged spheres imbedded in a polarizable
dielectric continuum. The defining equations of the Generalized
Born theory are as follows:
Equation 1 expresses the total electrostatic free energy G
es
of a
molecular system in kcal/mol as a sum of the Coulomb
interaction energies between each pair of charges q
i
and q
j
separated by a distance r
ij
in a solvent of dielectric constant ǫ
(the first term) and the Born solvation (self) energy of each
individual charge (the second term). The R
i
in eq 1 are the
Born radii, which are treated as disposable parameters. In eq
2, the free energy is rewritten as a sum of Coulomb interaction
energies in a vacuum and polarization free energy G
pol
. The
GB polarization energy captures all the electrostatic effects due
to solvent in one single term (eq 3), with a judicious choice of
the effective distance parameter f
GB
as provided by eq 4. The
* Author for correspondence. E-mail: dbeveridge@wesleyan.edu. Fax:
(860) 685-2211. Tel.: (860) 685-2575.
†
On leave from Department of Chemistry, Indian Institute of Technology,
Hauz Khas, New Delhi 110016, India.
9571 J. Phys. Chem. B 1998, 102, 9571-9576
10.1021/jp982007x CCC: $15.00 © 1998 American Chemical Society
Published on Web 11/03/1998
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