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2015
DOI: 10.1016/j.electacta.2015.06.145
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An analytical longitudinal dielectric function of primitive electrolyte solutions and its application in predicting thermodynamic properties

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Cited by 11 publications
(12 citation statements)
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“…Most of these approximations have been used to obtain thermodynamical quantities, distribution functions and/or the mean electrostatic potential. 15,16,27,28,[31][32][33]37,39,[42][43][44][45][46][47] Xiao and Song [48][49][50] have developed a linear theory that exploits all decay modes obtained in many of these approximations to calculate thermodynamical quantities for electrolytes. We will return to some of these linear, approximate theories later.…”
Section: Brief Overview Of Electrolyte Theories and Screeningmentioning
confidence: 99%
“…Most of these approximations have been used to obtain thermodynamical quantities, distribution functions and/or the mean electrostatic potential. 15,16,27,28,[31][32][33]37,39,[42][43][44][45][46][47] Xiao and Song [48][49][50] have developed a linear theory that exploits all decay modes obtained in many of these approximations to calculate thermodynamical quantities for electrolytes. We will return to some of these linear, approximate theories later.…”
Section: Brief Overview Of Electrolyte Theories and Screeningmentioning
confidence: 99%
“…Our MDH theory is applicable to the solutes with general geometry and charge density and has been tested for several systems. [25][26][27][28] With the above excess properties, it is possible to evaluate other thermodynamic properties of an electrolyte solution. The averaged excess internal energy per particle is…”
Section: F Electrostatic Contributions To Thermodynamic Properties: IImentioning
confidence: 99%
“…Note that χ(k) in most case is not analytically known, an empirical function χ(k) = a 0 k 2 k 4 + (a 1 k 2 − a 2 )Cos(kb) + a 3 Sin(kb) + a 2 can be used to fit the response function χ(k), and then the pole k = ik n can be determined by solving k 4 + (a 1 k 2 a 2 )Cos(kb) + a 3 Sin(kb) + a 2 = 0 numerically. 27,28 (2) The hard sphere contribution to the charge density ρ hs j (k) = n i q i x i h hs ij (k) can be evaluated using the analytical correlation function h hs ij (k) from the Percus-Yevick (PY) theory or other integral equation theory for hard sphere mixtures, 15 and then the cumulate charge Q hs j ≡ ∫ ρ hs j (r)4πr 2 dr and the electric potential ψ hs j ≡ ∫ ρ hs j (r) r 4πr 2 dr can be determined. The parameters ρ hs e and a d of the effective surface charge are evaluated by ρ hs e = (ψ hs j ) 2 /(4πQ hs j ) and a d = Q hs j /ψ hs j .…”
Section: G Prescriptions To Determine the Linear Coefficient {C As mentioning
confidence: 99%
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“…from MD simulation is fitted to a half empirical function [52][53][54] which is the function form of the MSA response function for a dipolar hard sphere fluid. The fitted parameters are found to be a 1 = 7.1953, a 2 = 120.58, a 3 = 10.431, a 4 = 619.04, b 1 = 3.2588, and b 2 = 0.300 96.…”
Section: Application To a Symmetric Diatomic Polar Fluidmentioning
confidence: 99%