2005
DOI: 10.5488/cmp.8.2.357
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Dielectric constant of the polarizable dipolar hard sphere fluid studied by Monte Carlo simulation and theories

Abstract: A systematic Monte Carlo (MC) simulation and perturbation theoretical (PT) study is reported for the dielectric constant of the polarizable dipolar hard sphere (PDHS) fluid. We take the polarizability of the molecules into account in two different ways. In a continuum approach we place the permanent dipole of the molecule into a sphere of dielectric constant ∞ in the spirit of Onsager. The high frequency dielectric constant ∞ is calculated from the Clausius-Mosotti relation, while the dielectric constant of th… Show more

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Cited by 17 publications
(13 citation statements)
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“…Assuming chaotic orientation under zero field, their reorientation and saturation under the applied field can be described by the introduction of an additional term into the CM equation (see Equation (13)) εnormaleffεmεnormaleff+2εm=n3ε0α+μd2kBTgKHere, the Kirkwood g ‐factor (gK in Equation (83)) accounts for the correlations between the dipoles at the Langevin level, and its correct value can be computed using molecular dynamics simulations. [ 150 ] Then, by using αnormaleff=α+μd2gK/false(kBTfalse) instead of α in Sections 3– 5, our theoretical model for the nanocomposite permittivity can be extended to include any permanent dipoles of the inclusions. Here, however, extra care should be taken for inclusion rotations which might affect the mechanical properties of the nanocomposite, as discussed in ref.…”
Section: Discussionmentioning
confidence: 99%
“…Assuming chaotic orientation under zero field, their reorientation and saturation under the applied field can be described by the introduction of an additional term into the CM equation (see Equation (13)) εnormaleffεmεnormaleff+2εm=n3ε0α+μd2kBTgKHere, the Kirkwood g ‐factor (gK in Equation (83)) accounts for the correlations between the dipoles at the Langevin level, and its correct value can be computed using molecular dynamics simulations. [ 150 ] Then, by using αnormaleff=α+μd2gK/false(kBTfalse) instead of α in Sections 3– 5, our theoretical model for the nanocomposite permittivity can be extended to include any permanent dipoles of the inclusions. Here, however, extra care should be taken for inclusion rotations which might affect the mechanical properties of the nanocomposite, as discussed in ref.…”
Section: Discussionmentioning
confidence: 99%
“…(142), and the broken curves give the CM [6,7], Onsager [9], and MSA [12] results. The points are simulation results [8].…”
Section: Clausius-mossotti Results Formentioning
confidence: 99%
“…Sometimes this problem is called the polarization catastrophe. The CM result for is plotted and compared with some simulation results [8] in figure 1. There is no singularity in the simulation results.…”
Section: Clausius-mossotti Results Formentioning
confidence: 99%
“…According to the Clausius‐Mosotti (C‐M) equation of dielectric polarization Pm=ɛ1ɛ+2×Mρ=NA3ɛ0×(αe+αa+αd) where Pm is the polarization, M is the relative molecular weight, ρ is the density of the material, and NA is the Avogadro's constant.…”
Section: Theoretical Analysismentioning
confidence: 99%
“…In the process of SBR's thermo-oxidative aging, a e barely changes from the external electric field which is much weaker than the electric field of the nucleus, so this part of the polarizability hardly changes in the THz field; a a is mainly caused by the deformation and twist of the atoms on the molecular-chain skeleton structure; a d is dependent on the fixed dipole moment and the polarity element. According to the Clausius-Mosotti (C-M) equation of dielectric polarization 36,37…”
Section: T Heor Eti Ca L Ana Lys I Smentioning
confidence: 99%