Jk. Hyun et al., APPARENT LOCAL DIELECTRIC RESPONSE AROUND IONS IN WATER - A METHOD FOR ITS DETERMINATION AND ITS APPLICATIONS, Journal of physical chemistry, 99(14), 1995, pp. 5187-5195
The solvation properties of ions in aqueous solution are determined by
the unique structure of water and its dielectric properties. The orie
ntational structure of the water molecules is governed in part by the
dipolar nature of water but displays a much richer behavior due to hyd
rogen bonding. Here, properties of the orientation angle theta of a wa
ter dipole as a function of distance r from the ion, namely, the mean
value [cos theta](r) and the distribution P(cos theta;r), are calculat
ed from molecular dynamics simulations of Cl- in water. The orientatio
nal behavior is compared to that of a point charge and a point dipole
in a dielectric continuum, which can be solved analytically. More spec
ifically, the microscopic field due to a point charge experienced by t
he dipole is different than the macroscopic field due to a point charg
e so that the problem must be viewed as a dipole in a cavity immersed
in a dielectric continuum, using arguments similar to those of Kirkwoo
d in relating the dielectric constant epsilon of a fluid to the dipole
moment mu of molecules in the fluid. By comparing (cos theta)(r) calc
ulated from simulation with the analytic expressions, an apparent ''lo
cal'' dielectric response epsilon(r) dependent on r is calculated; eps
ilon(r) is termed apparent because it is not a position-dependent diel
ectric constant to be used in the Poisson or Poisson-Boltzmann equatio
ns but rather reflects the cumulative effects of such a position-depen
dent dielectric constant. The variation of epsilon(r) from the bulk di
electric constant allows one to quantitate the deviations from continu
um behavior. In the first two shells, epsilon(r) varies significantly
with r, and a reduction in epsilon(r) in the first shell is clearly se
en. Furthermore, epsilon(r) appears to appl:oach continuum bulk behavi
or by about 8 Angstrom despite the considerable orientation even at r
= 10 Angstrom. In addition, the simple expression for P(cos theta;r) i
n the continuum approximation using epsilon(r) is used to calculate so
lvation properties of ions. It is also demonstrated that, in the limit
where epsilon(r) is assumed constant (i.e., that of bulk) and the den
sity is assumed constant (i.e., a continuum), the Born solvation energ
y expression is a limiting case of our expression for the solvation en
ergy.