A critical analysis of methods of calculation of a potential in simulated polar liquids: Strong arguments in favor of "molecule-based" summation and of vacuum boundary conditions in Ewald summation
Yn. Vorobjev et J. Hermans, A critical analysis of methods of calculation of a potential in simulated polar liquids: Strong arguments in favor of "molecule-based" summation and of vacuum boundary conditions in Ewald summation, J PHYS CH B, 103(46), 1999, pp. 10234-10242
The calculation of the electrostatic potential inside a polar liquid in an
infinitely large system simulated with periodic boundary conditions allows
several alternative choices for carrying out the summation over all particl
es. For a summation of contributions from charge centers limited to the con
tents of a sphere surrounding the point where the potential is calculated,
the cutoff can be based on the location of individual charge centers (so-ca
lled q-based summation) or on the location of molecular centers (M-based su
mmation); these two methods have been found to provide consistently differe
nt values of the potential. On the other hand, for a summation based on the
Ewald method, the choice of the latter's boundary conditions ("vacuum" ver
sus "tinfoil") affects the value of the calculated potential. A recent disc
ussion did not lead to a conclusion as to which is the right choice. Here,
we provide a new analysis of M- and q-based cutoff methods and show the fol
lowing. (i) The M-based method is the correct method to calculate the Coulo
mbic average potential exerted by a polar molecular liquid in the center of
a Lennard-Jones (LJ) solute. (ii) Each solute-solvent force field is chara
cterized by a unique M-center for which the potential is zero in the high-t
emperature limit. This unique M-center is the center of the solvent-solute
hard-core interaction for which the solvent molecule's orientational phase
space is uncoupled from its positional phase space in the rotational high-t
emperature limit. (iii) The best value of the average Coulomb potential of
water solvent inside a "methane" LJ solute in SPC water at T = 300 K and P
= 1 bar is negative, of the order of -7 to -8 kcal/(mol.e); this includes a
uniform potential of the order of +2 to +3 kcal/ (mol.e) produced by the p
olarized surface of the outer liquid--vapor interface of a macroscopic drop
let. (iv) The q-based method of calculation of the potential violates the s
elf-consistency of statistical sampling of the configurations of charged si
tes of the solvent molecules. (v) The effective M- or q-based potentials ca
lculated with Ewald "vacuum" potential are equal to the respective Coulombi
c potentials. (vi) Use of "tinfoil" boundary conditions for the Ewald poten
tial overestimates the interaction of the central cell with its surrounding
s and enhances periodicity, and is therefore less appropriate for simulatio
ns of liquid systems.