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Microscopic fields in liquid dielectrics
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10.1063/1.3006313
/content/aip/journal/jcp/129/17/10.1063/1.3006313
http://aip.metastore.ingenta.com/content/aip/journal/jcp/129/17/10.1063/1.3006313
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(a) Onsager’s directing field inside a dipolar liquid and the (b) cavity field inside a physical cavity carved in the liquid placed in the uniform external field . The local field [Eq. (3)] is a mean-field approximation for . is the dipole moment of a target molecule.

Image of FIG. 2.
FIG. 2.

Longitudinal (L) and transverse (T) structure factors of the dipolar hard-sphere liquid from numerical simulations at and (solid lines, ) and 1.0 (dashed lines, ).

Image of FIG. 3.
FIG. 3.

Response functions (dashed lines) and (dashed-dotted line) calculated from Eq. (22) and compared to [solid line, see Eqs. (25) and (26)]. The upper curves are obtained at , , while the lower curves refer to , ; . The and projections required for the integration in Eq. (22) have been obtained from MC simulations. Panels (a) and (b) correspond to and 1.5, respectively.

Image of FIG. 4.
FIG. 4.

Cavity field calculated from Eq. (31) with two cavity sizes indicated by the distance of the closest approach, , in the plot. The points were obtained by numerical integration in Eq. (31) with from MC simulations , while the dashed lines refer to the calculations using the parametrized MSA (Ref. 31). The integral is calculated numerically before the appearance of the singularity on the real axis [Eq. (35)] and by summation over the poles when the singularity falls on the axis. The two methods give identical results when numerical integration is justified. The upper and lower solid lines refer to two continuum limits, Eqs. (34) and (32), respectively. The dashed-dotted line refers to the lattice summation [Eq. (36)] instead of continuous integration in Eq. (31) taken for a cubic cell of , .

Image of FIG. 5.
FIG. 5.

The inverse dielectric susceptibility vs . The points represent simulation data. The solid line refers to Eq. (51), and the dotted line refers to Eq. (50). The remaining two lines are the continuum results obtained from the Debye and Onsager equations, Eqs. (6) and (8), respectively. The solid line is obtained by fitting the parameter in Eq. (51) to the simulation data with the best-fit value of .

Image of FIG. 6.
FIG. 6.

The depolarization coefficient as a function of the dielectric constant for a dipolar fluid at . The solid line is the fit to the simulation data (points) to Eq. (52). The dashed line is the Onsager result in Eq. (7).

Image of FIG. 7.
FIG. 7.

The cavity field calculated from MC simulations with varying cavity size: (, circles), 1.5 (, squares), 2.0 (, left triangles), 3.0 (, right triangles), and 5.5 (, up triangles). The solid line corresponds to the new continuum expression given in Eq. (34), while the dashed line refers to the standard Maxwell result [Eq. (32)].

Image of FIG. 8.
FIG. 8.

The cavity field calculated directly from simulations [Eq. (48)] as a function of the cavity radius . The insrt is an expanded section at large . The points represent (circles), 1.0 (squares), 2.0 (diamonds), and 3.0 (up triangles). The corresponding values of are 3.54, 8.52, 30.64, and 93.66.

Image of FIG. 9.
FIG. 9.

The correlator from Eq. (48) calculated from MC simulations for the dipoles in the first solvation shell surrounding the cavity (circles), from the second solvation shell (squares), and from the entire simulation box (open triangles). The sum of contributions from the first and second solvation shells is indicated by open diamonds. The cavity radius is .

Image of FIG. 10.
FIG. 10.

Reaction field calculated from the continuum electrostatics [Eq. (40)] (solid line marked “Onsager,” is used for the cavity radius) and from Eq. (39) (filled points) with the effective radius [Eq. (41)] used in place of : (circles), 1.0 (squares), and 1.5 (triangles). The open points correspond to the MC simulation data for the same values as the closed points. The dotted line applies Eq. (39) at with used for the cavity radius. The dashed lines connect the points and the structure factors from MC simulations were used for integration in Eq. (39).

Image of FIG. 11.
FIG. 11.

Microscopic field at the position of the dipole at the center of a spherical cavity of radius . The results at different were obtained for (circles), 1.0 (squares), and 1.5 (diamonds) using Eq. (49). The solid line refers to the continuum prediction for the homogeneous liquid [Eq. (46)], while dashed and dashed-dotted lines refer to and , respectively, obtained from Eq. (47).

Image of FIG. 12.
FIG. 12.

The local field [Eq. (3)] (circles), the cavity field (squares), and the directing field (closed triangles) vs for . The solid line indicates the new continuum cavity field [Eq. (34)], the dashed line is the Lorentz local field [Eq. (5)], and the dashed-dotted line is the Maxwell cavity field [Eq. (9)]. The lower panel is an expanded section at small .

Image of FIG. 13.
FIG. 13.

Directing field vs the target dipole moment . Points are simulations data at , ; the dotted line connects the points.

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/content/aip/journal/jcp/129/17/10.1063/1.3006313
2008-11-06
2014-04-18
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Microscopic fields in liquid dielectrics
http://aip.metastore.ingenta.com/content/aip/journal/jcp/129/17/10.1063/1.3006313
10.1063/1.3006313
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