posted on 2013-01-08, 00:00authored byAleksandr
V. Marenich, Christopher J. Cramer, Donald G. Truhlar
We present a new self-consistent reaction-field implicit
solvation
model that employs the generalized Born approximation for the bulk
electrostatic contribution to the free energy of solvation. The new
solvation model (SM) is called SM12 (where ″12″ stands
for 2012), and it is available with two sets of parameters, SM12CM5
and SM12ESP. The SM12CM5 parametrization is based on CM5 partial atomic
charges, and the SM12ESP parametrization is based on charges derived
from a quantum-mechanically calculated electrostatic potential (ESP)
(in particular, we consider ChElPG and Merz–Kollman–Singh
charges). The model was parametrized over 10 combinations of theoretical
levels including the 6-31G(d) and MG3S basis sets and the B3LYP, mPW1PW,
M06-L, M06, and M06-2X density functionals against 2979 reference
experimental data. The reference data include 2503 solvation free
energies and 144 transfer free energies of neutral solutes composed
of H, C, N, O, F, Si, P, S, Cl, Br, and I in water and in 90 organic
solvents as well as 332 solvation free energies of singly charged
anions and cations in acetonitrile, dimethyl sulfoxide, methanol,
and water. The advantages of the new solvation model over our previous
generalized Born model (SM8) and all other previous generalized Born
solvation models are (i) like the SMD model based on electron density
distributions, it may be applied with a single set of parameters with
arbitrary extended basis sets, whereas the SM8 model involves CM4
or CM4M charges that become unstable for extended basis sets, (ii)
it is parametrized against a more diverse training sets than any previous
solvation model, and (iii) it is defined for the entire periodic table.