A simple approach for calculating hydrogen bonding (H-bonding) effects in m
olecular mechanics simulations of peptides and proteins is presented for us
e in the framework of the continuum solvent model described in the previous
paper. In this approach, the solvated macromolecule is treated as a three-
component dielectric system consisting of the solvent, bulk protein, and pr
oton acceptor media. The hydrogen bond (H-bond) interaction is identified f
rom the interpenetration of the van der Waals spheres of the polar hydrogen
and the proton acceptor. The H-bond geometry is characterized by the ideal
orientation of the electron lone pairs in the acceptor atom and the direct
ionality of the proton donor bond, as observed in experimental and ab initi
o studies, and classified according to the hybridization state of the accep
tor atom. The algorithm was implemented into CHARMM using the PAR22 force f
ield. By introducing the concept of a Born radius of a polar hydrogen immer
sed in an acceptor environment, the stabilization of H-bond energies can be
introduced by means of a simple fitting procedure. This H-bonding descript
ion is easily implemented in standard force fields, with virtually no addit
ional computing time requirements. Monte Carlo simulations were carried out
on two peptides with this H-bonding treatment and the continuum solvent mo
del. The results clearly demonstrate the need for an explicit treatment of
H-bonding with the proposed continuum model, and its reliability to predict
peptide structures from the primary sequence that are in agreement with ex
perimental results.