Thermodynamics of a charged hard sphere in a compressible dielectric fluid. 2. Calculation of the ion-solvent pair correlation function, the excess solvation, the dielectric constant near the ion, and the partial molar volume of the ion in a water-like fluid above the critical point

1985 ◽  
Vol 89 (2) ◽  
pp. 380-384 ◽  
Author(s):  
Jacques R. Quint ◽  
Robert H. Wood
Keyword(s):  
Dielectric Constant ◽  
Correlation Function ◽  
Critical Point ◽  
Molar Volume ◽  
Partial Molar Volume ◽  
Pair Correlation Function ◽  
Hard Sphere ◽  
Pair Correlation ◽  
Dielectric Fluid

scholarly journals Pair correlation function characteristics of nearly jammed disordered and ordered hard-sphere packings

2005 ◽  
Vol 71 (1) ◽  
Author(s):  
Aleksandar Donev ◽  
Salvatore Torquato ◽  
Frank H. Stillinger
Keyword(s):  
Correlation Function ◽  
Pair Correlation Function ◽  
Hard Sphere ◽  
Pair Correlation ◽  
Sphere Packings

Ring approximation at equilibrium: The hard sphere pair correlation function

2007 ◽  
Vol 379 (2) ◽  
pp. 409-416 ◽  
Author(s):  
Jarosław Piasecki ◽  
Rodrigo Soto
Keyword(s):  
Correlation Function ◽  
Pair Correlation Function ◽  
Hard Sphere ◽  
Pair Correlation ◽  
Ring Approximation

Pair correlation function of inhomogeneous hard sphere fluids

1998 ◽  
Vol 150-151 ◽  
pp. 565-571 ◽  
Author(s):  
B. Götzelmann ◽  
S. Dietrich
Keyword(s):  
Correlation Function ◽  
Pair Correlation Function ◽  
Hard Sphere ◽  
Pair Correlation

Decay of pair correlation functions

1977 ◽  
Vol 55 (9) ◽  
pp. 761-766 ◽  
Author(s):  
Yoshio Tago ◽  
William R. Smith
Keyword(s):  
Correlation Function ◽  
Correlation Length ◽  
Correlation Functions ◽  
Pair Correlation Function ◽  
Hard Sphere ◽  
Pair Correlation ◽  
Direct Correlation Function ◽  
Pair Correlation Functions ◽  
Hard Sphere Fluid

The decay equation, which determines the correlation length and the period of the pair correlation function of a fluid at large distances, is discussed using the Ornstein–Zernike equation when the direct correlation function vanishes rapidly at large distances. The decay equation is solved numerically using the exact hard sphere and sticky hard sphere fluid results from the Percus–Yevick approximation. In the case of the hard sphere fluid, oscillatory decay is always obtained. For the sticky hard sphere fluid, we obtain a locus both in the pressure–temperature plane and the density–temperature plane such that the decay is monotonic inside and oscillatory outside the locus.

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